6533b85efe1ef96bd12c05e5

RESEARCH PRODUCT

Experimental study of the halo nucleusHe6using theLi6(γ,π+)He6reaction

J. R. M. AnnandK. FöhlI. J. D. MacgregorD. BranfordS. WaddellD. P. WattsF. MoschiniIan MartinIan MartinA. ReiterK. LivingstonP. GrabmayrR. BeckD. HornidgeT. HehlE. RocheN. P. HarringtonK. MonstadJ. C. McgreorgeStuart Young

subject

PhysicsNuclear and High Energy PhysicsPhotonPionExcited stateIsotopes of lithiumBremsstrahlungHalo nucleusHaloAtomic physicsNuclear ExperimentGround state

description

The reaction $^{6}\mathrm{Li}$($\ensuremath{\gamma},{\ensuremath{\pi}}^{+})$$^{6}\mathrm{He}$ was studied over the angular range ${\ensuremath{\theta}}_{\ensuremath{\pi}}=40$--150$\ifmmode^\circ\else\textdegree\fi{}$ with the aim of investigating the halo structure of $^{6}\mathrm{He}$. Photons from a bremsstrahlung beam were tagged in the energy range ${E}_{\ensuremath{\gamma}}=170$--220 MeV at a resolution of $\ensuremath{\Delta}{E}_{\ensuremath{\gamma}}=630$ keV, and positively charged pions detected using high resolution stacked HpGe detectors. The measured angular distributions for the resolved $^{6}\mathrm{He}$ ground and 1.80 MeV excited states are compared to previous measurements and theoretical calculations based on the impulse approximation. It is deduced that the ground state rms radius of the $^{6}\mathrm{He}$ nucleus may be larger than previously thought and that the first excited 1.80 MeV state may also be a halo state.

https://doi.org/10.1103/physrevc.75.044311